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The physical interpretation of the activation energy for hot deformation of Ni and Ni-30Cu alloys

机译:Ni和Ni-30Cu合金热变形活化能的物理解释

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摘要

Hot compression tests on pure Ni and Ni-30Cu at 950-1150 ℃ and strain rates of 0.001-1 s~(-1) were performed to identify the physical interpretation of the apparent activation energy (Q_d). For pure Ni, Q_d was constant and identical to that of the self-diffusion. However, for Ni-30Cu, it decreased steadily with strain. The value of Q_d was separated into thermal and mechanical parts. The thermal part was necessary to propel diffusion. For pure Ni, the mechanical part was zero at low and medium strain rates of 0.001-0.1 s~(-1) and the self-diffusion was the controlling mechanism. However, at 1 s~(-1) both the thermal and mechanical parts were needed to provide Q_d. For Ni-30Cu, Q_d was greater than that for the interdiffusion of Ni and Cu. The value of mechanical part decreased with increasing temperature and strain rate. Although the thermal parts for pure Ni and Ni-30Cu were nearly identical, the mechanical part for the latter was considerably higher. The difference was attributed to the strengthening effect of Cu atoms and the sluggish dynamic softening with respect to pure Ni.
机译:在950-1150℃对纯Ni和Ni-30Cu进行热压缩试验,并在0.001-1 s〜(-1)的应变速率下进行热压缩试验,以确定表观活化能(Q_d)的物理解释。对于纯Ni,Q_d恒定且与自扩散相同。但是,对于Ni-30Cu,其随着应变而稳定降低。 Q_d的值分为热部分和机械部分。散热部分是推动扩散所必需的。对于纯Ni,在0.001-0.1 s〜(-1)的中低应变速率下,机械零件为零,并且自扩散是控制机理。然而,在1 s〜(-1)时,热和机械部件都需要提供Q_d。对于Ni-30Cu,Q_d大于Ni和Cu互扩散的Q_d。机械零件的值随着温度和应变率的增加而降低。尽管纯Ni和Ni-30Cu的热部分几乎相同,但后者的机械部分要高得多。差异归因于铜原子的增强作用和相对于纯镍的缓慢的动态软化。

著录项

  • 来源
    《Journal of Materials Research》 |2016年第8期|1077-1084|共8页
  • 作者

    Amir Momeni;

  • 作者单位

    Materials Science and Engineering Department, Hamedan University of Technology, Hamedan 6516913733, Iran;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
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